Startseite Existence results for nonlinear degenerate elliptic equations with lower order terms
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Existence results for nonlinear degenerate elliptic equations with lower order terms

  • Weilin Zou EMAIL logo und Xinxin Li
Veröffentlicht/Copyright: 2. August 2020

Abstract

In this paper, we prove the existence and regularity of solutions of the homogeneous Dirichlet initial-boundary value problem for a class of degenerate elliptic equations with lower order terms. The results we obtained here, extend some existing ones of [2, 9, 11] in some sense.

MSC 2010: 35D30; 35J60; 35J70

1 Introduction

Recently, much attention has been payed to partial differential equations with lower order terms, not only for their physical relevance but also for their mathematical interest. From the mathematical point of view, it is well known that the lower order terms may affect the existence, uniqueness, regularity and asymptotic behavior of solutions to partial differential equations (see e.g. [1, 3, 4, 5, 6, 7, 8, 9, 10, 11, 12, 19, 23]). In this paper, we are interested in the existence and regularity of solutions for a class of degenerate elliptic equations with two lower order terms, whose prototype is

(P~)div(a(x,u)|u|p2u(1+|u|)θ(p1))+ν|u|t1u=y|u|pr+finΩ,u=0onΩ,

where Ω is a bounded open subset of ℝN(1 < p < N), a(x, s) is a Carathéodory matrix and f is a measurable function.

As θ = 0, such kind of problems with different lower order terms were studied well in the literature. Without the aim to be complete, let us mention the following revelent works. The quasi-linear case p = 2 was treated in [9], where it was shown that the term νut−1u was in some sense to guarantee the existence of a solution when the growth of the gradient is superlinear. If there was an L1 interplay between the coefficient of the zero order term and the right-hand side f, the existence of bounded solutions was established in [4]. This result was improved in [5] and extended to the parabolic case in [16]. If p = 2, a(x, s) was an identity matrix, f = 0 and y = 0, the existence and non-existence results to problem (𝒫̃) with two zero order terms were proved in [12]. The case ν = 0 was considered in [1], where it was proved that smallness condition was asked on f to guarantee the existence of a solution. For other related results, see [3], where the existence, multiplicity and non-existence of solutions to a semilinear degenerate elliptic system of Hamiltonian type were proved; see also [19], where a Neumann problem driven by the p-Laplacian with singular and convection terms was investigated.

As θ ≠ 0, it is easy to see that the principal part of problem (𝒫̃) degenerates, hence, a slow diffusion effect may appear as soon as the solution u becomes large. Such kind of equations could be seen as a reaction model which produces a saturation effect. In case of ν = y = 0, existence and regularity results of problem (𝒫̃) were established in [2, 13], while the parabolic case of such problem was just treated in [15](see also [21]). We also mention that the related obstacle problems with L1 data were investigated in [24, 25].

When p = 2 and y = 0, the author in [11] proved that the zero order term νut−1u may affect the regularity of solutions of (𝒫̃) under the assumption that fLm(Ω) with m ≥ 1. This result was extended to the general case p > 1 in [10]. For this general case, the stability results were obtained in [14]. Also, it was shown in [7] that the existence of W01,1 (Ω) solutions could be obtained by adding a zero order term. For other relevant papers, see [18, 22] and the references therein.

Motivated by [2, 9, 11], this work studies the regularizing effect of lower order terms on the solutions to problem (𝒫̃) (that is ν ≠ 0 and y ≠ 0). The main results obtained here generalize the previous result of [2, 9, 11] in some sense. The main difficulties are the facts that the differential operator is not coercive on W01,p (Ω) and the lower order terms have regularizing effects on solutions. To overcome these difficulties, we shall first introduce a class of approximated problems and then establish some estimates for solutions by taking suitable test functions, and finally prove some convergence results to get the existence results.

This paper is organized as follows. In Section 2, we give the assumptions and the main results. In Section 3, we shall prove the main results.

2 Assumptions and the main results

Let Ω be a bounded open subset of ℝN with N ≥ 2, 1 < p < N. Throughout this paper, ci or i (i = 0, 1, 2 … n) will denote a positive constant which only depends on the parameters of our problem. For any real number η > 1, we set η=ηη1 and η=NηNη. For EΩ, we also denote

Eg:=Egdx,|E|=measE.

We shall use the truncation functions Tk(s) and Gk(s) defined by

Tk(s)=max{k,min{k,s}},Gk(s)=sTk(s).

Let us consider the following problem:

(P)div(a(x,u,u))+g(x,u)=b(x,u,u)+fdivFinΩ,u=0onΩ,

where a : Ω × ℝ × ℝN → ℝN, b : Ω × ℝ × ℝN → ℝ and g : Ω × ℝ → ℝ are Carathéodory functions satisfying:

There exist constants α, β, ν, y ∈ ℝ+, and a nonnegative function jLp(Ω) such that

a(x,s,ξ)ξα(1+|s|)θ(p1)|ξ|p,with0θ<1, (2.1)
|a(x,s,ξ)|β[j(x)+|s|p1+|ξ|p1], (2.2)
[a(x,s,ξ)a(x,s,ζ)][ξζ]>0, (2.3)
|b(x,s,ξ)|y|ξ|pr,withmax{p1p,1p}<r<1, (2.4)
g(x,s)sν|s|t+1,witht>r+θr(p1)1r, (2.5)

for almost every xΩ, for every s ∈ ℝ and for every ξ, ζ ∈ ℝN with ξζ.

Now we give the definition of weak solutions to problem (𝒫).

Definition 2.1

A measurable function u W01,1 (Ω) is called a weak solution of problem (𝒫), if a(x, u, ∇ u), g(x, u) and b(x, u, ∇ u) are summable functions and

Ωa(x,u,u)ϕ+Ωg(x,u)ϕ=Ωb(x,u,u)ϕ+Ωfϕ+ΩFϕϕD(Ω). (2.6)

The main results of this paper are stated as follows.

Theorem 2.1

Suppose that assumptions (2.1)-(2.5) hold with fL1(Ω) and F (Lpt(p1)(tθ)(Ω))N , then there exists at least a weak solution u W01,q (Ω) ∩ Lt (Ω) of the problem (𝒫) for every 1 ≤ q < q1, where q1=max{ptt+1+θ(p1),N(p1θ(p1))N1θ(p1)}.

Remark 2.1

The assumption F (Lpt(p1)(tθ)(Ω))N imposed here is to get the result (3.10) and then to obtain the existence result, see step 2 of the proof of Theorem 2.1. However to get the regularity result u W01,q (Ω) ∩ Lt(Ω), it suffices to assume that F (Lpp1(Ω))N, see step 1 of the proof of Theorem 2.1. If θ = 0 and p = 2, the assumption F (Lpt(p1)(tθ)(Ω))N reduces to F ∈ (L2(Ω))N, which coincides the result of [9].

Remark 2.2

By (2.4) and (2.5) it easy to check that ptt+1+θ(p1) > 1 which implies that q1 > 1. We remark that the restriction of (2.4) listed here is to simplify the proof and can be replaced by 1p < r < 1. Indeed, using Young’s inequality, it is easy to see that the above assertion remains true and our results in Theorem 2.1 and Theorem 2.2(see below) are still true in the case that 1p < r < 1. Thus our results Theorem 2.1 and Theorem 2.2 also cover the results of [9] where θ = 0 and p = 2.

Theorem 2.2

Suppose that (2.1)-(2.5) hold, and fLm(Ω), where 1 < m < Np.

  1. If F = 0, then there exists at least a weak solution uW01,q(Ω)Ltm(Ω)Lmp(p1)(1θ)mpp(Ω) of the problem (𝒫) where q=minp,maxptmt+1+θ(p1),pmp(p1)(1θ)(p1)[p(m1)+θm(pp)]+mpp. Thus if t(m − 1) − θ (p − 1) − 1 ≥ 0   or if Np(1θ)[N(p1)+p]+p2θ<m<Np, then u W01,p (Ω).

  2. If F ≠ 0, let us assume that F ∈ (Lb(Ω))N. Then there exists a weak solution u W01,q2 (Ω) ∩ L^{tm}(Ω), where bb0=maxpt(p1)(tθ),ptm(p1)(t+1θ)andq2=minp,ptmt+1+θ(p1).

    In the case that bb1=maxpt(p1)(tθ),pp1tt+1θ+p(p1)(1θ)(t+1θ)(pmp), there exists at least a weak solution uW1,q3(Ω) ∩ Lmp(p1)(1θ)mpp (Ω), where q3=minp,pmp(p1)(1θ)(p1)[p(m1)+θm(pp)]+mpp.

    Finally, denoting q = max{q2, q3}, if b ≥ max{b0, b1}, then there exists at least a solution u W01,q (Ω) ∩ Ltm(Ω) ∩ Lmp(p1)(1θ)mpp (Ω).

3 Proof of the main results

In order to prove the existence results, let us define

bn(x,s,ξ)=b(x,s,ξ)1+1n|b(x,s,ξ)|,fn(x)=f(x)1+1n|f(x)|,Fn(x)=F(x)1+1n|F(x)|. (3.1)

We consider the following approximated problems

Ωa(x,Tn(un),un)φ+Ωg(x,un)φ=Ωbn(x,un,un)φ+Ωfnφ+ΩFnφ,φW01,p(Ω)L(Ω). (3.2)

The existence of weak solution un W01,p (Ω) of (3.2) follows by the classical result of [17].

3.1 Proof of Theorem 2.1

The proof relies on an approximation procedure which is divided into several steps.

  1. We prove the following a priori estimates:

    Ω|un|tc0andΩ|un|qc0, (3.3)
    Ω|Gk(un)|qϵ(k), (3.4)

    for 1 ≤ q < q1, where ϵ(k) does not depend on n and tends to zero when k tends to +∞.

    To prove the above estimates, we take φ = [1 − (1 + ∣un∣)1−λ]sgn(un) as a test function in (3.2), where λ > 1 will be chosen later. Using Young’s inequality, it leads to

    α(λ1)Ω|un|p(1+|un|)θ(p1)+λ+νΩ|un|t[1(1+|un|)1λ]α(λ1)2Ω|un|p(1+|un|)θ(p1)+λ+y11rα2(λ1)r/(1r)Ω(1+|un|)θr(p1)+λr1r+Ω|f|+α(λ1)4Ω|un|p(1+|un|)θ(p1)+λ+(λ1)4α1p1Ω|F|pp1. (3.5)

    Choosing S > 0 such that 1 − (1 + S)1−λ = 1/2, we easily obtain

    12Ω|un|t12{xΩ:|un|S}|un|t+12{xΩ:|un|>S}|un|t12St|Ω|+Ω|un|t[1(1+|un|)1λ].

    The above inequality together with (3.5) imply that

    α(λ1)4Ω|un|p(1+|un|)θ(p1)+λ+ν2Ω|un|ty11rα2(λ1)r/(1r)Ω(1+|un|)θr(p1)+λr1r+Ω|f|+ν2St|Ω|+(λ1)4α1p1Ω|F|pp1. (3.6)

    Observing that t > [r + θ r(p − 1)]/(1 − r) (see (2.5)), one may choose λ in (3.6) such that [θ r(p − 1) + λ r]/(1 − r) < t, i.e. 1 < λ < [t(1 − r) − θ r(p − 1)]/r. Hence, we get

    Ω|un|p(1+|un|)θ(p1)+λc1andΩ|un|tc1. (3.7)

    Therefore by the two estimates of (3.7), we infer that for qptθ(p1)+λ+t<ptθ(p1)+1+t, it results (θ(p − 1) + λ)q/(pq) ≤ t and so

    Ω|un|qΩ|un|q(1+|un|)(θ(p1)+λ)q/p(1+|un|)(θ(p1)+λ)q/pc1qpΩ(1+|un|)(θ(p1)+λ)q/(pq)1qpc2. (3.8)

    Setting q~=N(pθ(p1)λ)Nθ(p1)λ and q0=N(pθp+θ1)Nθp+θ1, obviously we have < q0.

    If q0 > 1, then by (2.1), (3.7) and taking 1 < λ < pθ(p − 1), we find that for 1 ≤ < q0,

    Cq~Ω|un|q~q~q~Ω|un|q~=Ω|un|q~(1+|un|)(θ(p1)+λ)q~/p(1+|un|)(θ(p1)+λ)q~pc1q~pΩ(1+|un|)q~1q~p,

    where C is the Sobolev constant and = (θ(p − 1) + λ) /(p). By the choice of 1 < λ < pθ(p − 1), we observe that / > 1 − /p. Thus by Young’s inequality we easily get

    Ω|un|q~c2for1q~<q0. (3.9)

    Taking 1 < λ < min{pθ(p − 1), [t(1 − r) − θ r(p − 1)]/r}, by (3.7), (3.8) and (3.9), we conclude that (3.3) holds for 1 ≤ q < q1 = max{ptt+1+θ(p1),q0}.

    If q0 ≤ 1, then (3.8) leads to (3.3) for 1 ≤ q < ptt+1+θ(p1). Therefore, for both case q0 ≤ 1 and q0 > 1, we conclude that (3.3) holds true.

    Finally, the proof of (3.4) is similar at all to that of (3.3), except that the test function is changed to φ = [1 − (1 + ∣Gk(un)1−λ∣)] sgn(Gk(un)), so we omit the detail here.

  2. we now prove the following convergence result:

    g(x,un)g(x,u)L1(Ω)0. (3.10)

    To do this, firstly it is easy to derive from the estimates (3.3) that for a subsequence of {un} (still denote by {un}), and a function u W01,q (Ω) ∩ Lt(Ω), such that as n → +∞ it results:

    unu a.e. in Ωand weaklyinW01,q(Ω)Lt(Ω). (3.11)

    Then for fixed l, d > 0, taking T11d(|un|l)+ sgn(un) as a test function in (3.2), we get by applying Young’s inequality and using (3.3),

    αd{xΩ:l|un|l+d}|un|p(1+|un|)θ(p1)+{xΩ:|un|l+d}|g(x,un)|α2d{xΩ:l|un|l+d}|un|p(1+|un|)θ(p1)+c3{xΩ:l|un|l+d}(1+|un|)θr(p1)1r+y{xΩ:|un|l+d}|un|pr+{xΩ:|un|l}|f|+α2d{xΩ:l|un|l+d}|un|p(1+|un|)θ(p1)+c4{xΩ:l|un|l+d}|F|pt(p1)(tθ)tθt,

    where c3=(1r)(2drα)r/(1r) and c4=1d(2pα)1p1p1pc0θt.

    By (2.5) and (3.3), we have

    c3A(l)(1+|un|)θr(p1)1rc3A(l)(1+|un|)tθr(p1)t(1r)|A(l)|t(1r)θr(p1)t(1r)c5|A(l)|t(1r)θr(p1)t(1r),

    where c5=2θr(p1)1rc0θr(p1)t(1r)c3 and A(l) = {xΩ : l ≤ ∣un∣ ≤ l + d}.

    The above two inequalities and (2.5) yield

    Ω|g(x,un)|=Ω|g(x,un)|χ{xΩ:0|un(x)|l+d}+{xΩ:|un|l+d}|g(x,un)|Ω|g(x,un)|χ{xΩ:0|un(x)|l+d}+ε(l), (3.12)

    where the term ε(l) satisfying liml+ ε(l) = 0 is denoted by

    ε(l)=yunW01,q(Ω)pr|{xΩ:|un|l+d}|qprq+{xΩ:|un|l}|f|+c5|A(l)|t(1r)θr(p1)t(1r)+c4A(l)|F|pt(p1)(tθ)tθt.

    By applying (3.12), Lebesgue’s dominated convergence theorem and Fatou lemma, it can be concluded that

    Ω|g(x,un)|Ω|g(x,u)|,asn+. (3.13)

    Combining (3.13) with (3.11), we obtain the desired result (3.10).

  3. End the proof.

    To do this, for any h > 0 let us take Th(un) as a test function in (3.2), we easily obtain that

    Ω|Th(un)|pc6hθ(p1)+1+c7. (3.14)

    Then there exists a subsequence (still denoted {un}) such that

    Th(un)Th(u)weaklyinW01,p(Ω). (3.15)

    Then use the argument of [20](see also [6, 8, 9]) one may get

    unua.e.inΩ. (3.16)

    By (3.14)-(3.16) and Fatou lemma, we conclude

    Ω|Th(u)|pc8andΩ|Th(un)Th(u)|pc9, (3.17)

    which gives

    kp|ΩEk,n|ΩEk,n|Th(un)Th(u)|pΩ|Th(un)Th(u)|pc9, (3.18)

    where Ek,n := {xΩ : ∣∇ Th(un)(x) − ∇ Th(u)(x)∣ ≤ k}. Then we obtain

    Ω|Th(un)Th(u)|q=Ek,n|Th(un)Th(u)|q+ΩEk,n|Th(un)Th(u)|qΩχEk,n|Th(un)Th(u)|q+c10kqp,

    where we have used the results (3.16)-(3.18) and Hölder inequality. Thus, we get

    limn+supΩ|Th(un)Th(u)|qc10kqpk>0,

    which implies that

    Ω|Th(un)Th(u)|q0n+.

    Combining this result with (3.4), we deduce that

    unustronglyinW01,q(Ω). (3.19)

    Let n → ∞ in (3.2), by (2.2), (2.4), (2.5), (3.11) and (3.19), it follows that u is a weak solution of problem (𝒫) in the sense of Definition 2.1. Thus, the proof of Theorem 2.1 is finished.□

3.2 Proof of Theorem 2.2

  1. we first prove the result when F = 0.

    Let us take φ = [(1 + ∣un∣)δ − 1]sgn(un) in (3.2), where δ > 0 will be chosen later. We get after using Hölder’s inequality and Young’s inequality,

    αδ2Ω|un|p(1+|un|)δ1θ(p1)+Ωg(x,un)[(1+|un|)δ1]sgn(un)c~0Ω(1+|un|)δr(δ1)+rθ(p1)1r+fLm(Ω)Ω(1+|un|)δm1m. (3.20)

    Observing that as lims+st[(1+s)δ1](1+s)δ+t=1, there exists S0 = S0(δ, t) > 0 such that

    st[(1+s)δ1](1+s)δ+t2,sS0.

    Thus, by (2.5) and (3.20), we obtain

    Ωg(x,un)[(1+|un|)δ1]sgn(un)ν2{xΩ:|un|>S0}(1+|un|)δ+t. (3.21)

    By (3.20), (3.21) and notice that t > [r + θ r(p − 1)]/(1 − r), we infer that

    αδ2Ω|un|p(1+|un|)δ1θ(p1)+ν2{xΩ:|un|>S0}(1+|un|)δ+tc~0{xΩ:|un|S0}(1+|un|)δr(δ1)+rθ(p1)1r+{xΩ:|un|>S0}(1+|un|)δr(δ1)+rθ(p1)1r+fLm(Ω)Ω(1+|un|)δm1mv4{xΩ:|un|>S0}(1+|un|)δ+t+c~1+fLm(Ω)Ω(1+|un|)δm1m. (3.22)

    By choosing δ m = δ + t (i.e.δ = t(m − 1) in (3.22), we have

    αδ2Ω|un|p(1+|un|)δ1θ(p1)+ν4{xΩ:|un|>S0}(1+|un|)tmν8{xΩ:|un|>S0}(1+|un|)tm+c~2, (3.23)

    which implies that

    Ω|un|p(1+|un|)t(m1)1θ(p1)c~3andΩ(1+|un|)tmc~3.

    Obversely, we have

    Ω|un|pc~3,if t(m1)θ(p1)10. (3.24)

    Similarly to (3.8), in the case t(m − 1) − θ(p − 1) − 1 < 0 we get

    Ω|un|q4c~4,withq4=min{p,ptmt+1+θ(p1)}. (3.25)

    To end this proof in case F = 0, we shall choose a different δ in (3.22). Indeed, similar to (3.21) we infer that for S1(independent of n) large enough,

    αδ2Ω|un|p(1+|un|)δ1θ(p1)=ppαδ2[δ1θ(p1)+p]pΩ(1+|un|)δ1θ(p1)+pp1pc~5|un|>S1(1+|un|)[δ1θ(p1)+p]pppp. (3.26)

    By (3.22) and (3.26), it follows that

    Ω(1+|un|)[δ1θ(p1)+p]ppppc~6+c~6Ω(1+|un|)δm1m. (3.27)

    Let us choose δm=[δ1θ(p1)+p]pp(i.e.δ=p(p1)(1θ)mpp), then we have δm=mp(p1)(1θ)mpp. Hence, applying Young’s inequality in (3.27), we get

    Ω|un|mp(p1)(1θ)mppc~7. (3.28)

    Substituting (3.28) into (3.22), we find

    Ω|un|p(1+|un|)δ1θ(p1)c~8,δ=p(p1)(1θ)mpp. (3.29)

    In the case that δ ≥ 1 + θ(p − 1) (i.e. m Np(1θ)[N(p1)+p]+p2θ), we have

    Ω|un|pc~8, (3.30)

    while in the case that δ < 1 + θ(p − 1)(that is m < Np(1θ)[N(p1)+p]+p2θ), combining (3.28) with (3.29) and arguing as in (3.8) we obtain

    Ω|un|q5c~9withq5=pmp(p1)(1θ)(p1)[p(m1)+θm(pp)]+mpp. (3.31)

    Finally, by (3.24), (3.25), (3.28), (3.30) and (3.31), arguing as in the step 2 and step 3 we conclude that the result of this theorem holds true when F = 0.

    If F ≠ 0, then in the right-hand side of (3.20) it contains also the following term

    δΩF(1+|un|)δ1un.

    Using Young’s inequality, we easily obtain that

    δΩF(1+|un|)δ1unαδ4Ω|un|p(1+|un|)δ1θ(p1)+δ4α1p1Ω|F|pp1(1+|un|)δ+θ1.

    Thus if δ ≤ 1 − θ we obtain

    δ4α1p1Ω|F|pp1(1+|un|)δ+θ1δ4α1p1Ω|F|pp1,

    while if δ > 1 − θ we obtain

    δ4α1p1Ω|F|pp1(1+|un|)δ+θ1ν16Ω(1+|un|)δ+t+c~10Ω|F|pp1δ+tδ+θ1.

    As we have said in Remark 2.1, to guarantee the convergence result (3.10), we should assume F (Lpt(p1)(tθ)(Ω))N. Observe that the assumption bb0 is equivalent to require that if δ ≤ 1 − θ with δ = t(m − 1), then F (Lpp1(Ω))N; while if δ > 1 − θ then F(Lptm(p1)(t+1θ)(Ω))N, where ptm(p1)(t+1θ)=pp1δ+tδ+θ1. Similarly, the assumption bb1 is equivalent to require that if δ ≤ 1 − θ with δ=p(p1)(1θ)mpp, then F(Lpp1(Ω))N; while if δ > 1 − θ then F(Lpp1δ+tδ+θ1(Ω))N. Thus if bb0, using the previous estimates and proceeding as in the case F = 0, we conclude that un is equibounded in W01,q2 (Ω) ∩ Ltm(Ω); while if b > b1 we can conclude that un is equibounded in W01,q3(Ω)Lmp(p1)(1θ)mpp(Ω). Hence the assert follows as before. This completes the proof.□


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Acknowledgment

This work was supported by the National Natural Science Foundation of China(no.11801259, no.11461048), the foundation of Education Department of Jiangxi Province(no.GJJ170604).

References

[1] N. Alaa and M. Pierre, Weak solutions of some quasilinear elliptic equations with data measures, SIAM J. Math. Anal. 24 (1993), no.1, 23-35.10.1137/0524002Suche in Google Scholar

[2] A. Alvino, L. Boccardo, V. Ferone, L. Orsina and G. Trombetti, Existence results for nonlinear elliptic equations with degenerate coercivity, Ann. Mat. Pura Appl. 182 (2003), no.1, 53-79.10.1007/s10231-002-0056-ySuche in Google Scholar

[3] C. T. Anh and B. K. My, Existence and non-existence of solutions to a Hamiltonian strongly degenerate elliptic system, Adv. Nonlinear Anal. 8 (2019), no. 1, 661-678.10.1515/anona-2016-0165Suche in Google Scholar

[4] D. Arcoya and L. Boccardo, Regularizing effect of the interplay between coefficients in some elliptic equations, J. Funct. Anal. 268 (2015), no.5, 1153-1166.10.1016/j.jfa.2014.11.011Suche in Google Scholar

[5] D. Arcoya and L. Boccardo, Regularizing effect of Lq interplay between coefficients in some elliptic equations, J. Math. Pures Appl. 111 (2018), no.9, 106-125.10.1016/j.matpur.2017.08.001Suche in Google Scholar

[6] P. Bénilan, L. Boccardo, T. Gallouët, R. Gariepy, M. Pierre and J. L. Vázquez, An L1 theory of existence and uniqueness of solutions of nonlinear elliptic equations, Ann. Sc. Norm. Super. Pisa 22 (1995), no.2, 241-273.Suche in Google Scholar

[7] L. Boccardo, G. Croce and L. Orsina, Nonlinear degenerate elliptic problems with W01,1 (Ω) solutions, Manuscripta. Math. 137 (2012), no.3-4, 419-439.10.1007/s00229-011-0473-6Suche in Google Scholar

[8] L. Boccardo and T. Gallouët, Nonlinear elliptic and parabolic equations involving measure data, J. Funct. Anal. 87 (1989), no.1, 149-169.10.1016/0022-1236(89)90005-0Suche in Google Scholar

[9] L. Boccardo and M. M. Porzio, Quasilinear elliptic equations with subquadratic growth, J. Differ. Equations 229 (2006), no.1, 367-388.10.1016/j.jde.2006.01.016Suche in Google Scholar

[10] G. Chen, Nonlinear elliptic equation with lower order term and degenerate coercivity, Math. Notes 93 (2013), no.1-2, 224-237.10.1134/S0001434613010240Suche in Google Scholar

[11] G. Croce, The regularizing effects of some lower order terms in an elliptic equation with degenerate coercivity, Rend. Mat. Appl. 27 (2007), 299-314.Suche in Google Scholar

[12] J. I. Díaz, J. Hernández and Y. Sh. Ilyasov, On the exact multiplicity of stable ground states of non-Lipschitz semilinear elliptic equations for some classes of starshaped sets, Adv. Nonlinear Anal. 9 (2020), no. 1, 1046-1065.10.1515/anona-2020-0030Suche in Google Scholar

[13] D. Giachetti and M. M. Porzio, Elliptic equations with degenerate coercivity: gradient regularity, Acta Math. Sinica. 19 (2003), no.2, 349-370.10.1007/s10114-002-0235-1Suche in Google Scholar

[14] S. Huang, Q. Tian, J. Wang and J. Mu, Stability for noncoercive elliptic equations, Electron. J. Differ. Equ. 2016 (2016), no. 242, 1-11.Suche in Google Scholar

[15] F. Li, Existence and regularity results for some parabolic equations with degenerate coercivity, Ann. Acad. Sci. Fenn-M. 37(2012), no.2, 605 -633.10.5186/aasfm.2012.3738Suche in Google Scholar

[16] Z. Li, Existence Result to a Parabolic Equation with Quadratic Gradient Term and an L1 Source, Acta Applicandae Mathematicae 163 (2019), no.1, 145-156.10.1007/s10440-018-0217-7Suche in Google Scholar

[17] J. L. Lions, Quelques méthodes de résolution des problèmes aux limites nonlinéaires, Dunod Gauthier-Villars, Paris, 1969.Suche in Google Scholar

[18] A. Mercaldo, I. Peral and A. Primo, Results for degenerate nonlinear elliptic equations involving a Hardy potential, J. Differ. Equations 251 (2011), 3114-3142.10.1016/j.jde.2011.07.024Suche in Google Scholar

[19] N. S. Papageorgiou, V. D. Rădulescu and D. D. Repovš, Positive solutions for nonlinear Neumann problems with singular terms and convection, J. Math. Pures Appl. 136(2020), 1-21.10.1016/j.matpur.2020.02.004Suche in Google Scholar

[20] A. Porretta and S. Segura de León, Nonlinear elliptic equations having a gradient term with natural growth, J. Math. Pures Appl. 85 (2006), no.3, 465-492.10.1016/j.matpur.2005.10.009Suche in Google Scholar

[21] M. M. Porzio and M. A. Pozio, Parabolic equations with non-linear, degenerate and spacetime dependent operators, J. Evol. Equ. 8 (2008), no.1, 31-70.10.1007/s00028-007-0317-8Suche in Google Scholar

[22] M. M. Porzio and F. Smarrazzo, Radon measure-valued solutions for some quasilinear degenerate elliptic equations, Ann. Mat. Pura Appl. 194 (2015), no.2, 495-532.10.1007/s10231-013-0386-ySuche in Google Scholar

[23] Z. Zhang, Two Classes of Nonlinear Singular Dirichlet Problems with Natural Growth: Existence and Asymptotic Behavior, Adv. Nonlinear. Stud. 20 (2020), no.1, 77-93.10.1515/ans-2019-2054Suche in Google Scholar

[24] J. Zheng, The obstacle problem for non-coercive equations with lower order term and L1-data, J. Inequal. Appl. 2019(2019), 205, 15pp.10.1186/s13660-019-2157-9Suche in Google Scholar

[25] J. Zheng and L. S. Tavares, The obstacle problem for nonlinear noncoercive elliptic equations with L1-data, Bound. Value Probl. 2019(2019), 53, 15pp.10.1186/s13661-019-1168-2Suche in Google Scholar

Received: 2019-07-17
Accepted: 2020-06-17
Published Online: 2020-08-02

© 2021 Weilin Zou and Xinxin Li, published by De Gruyter

This work is licensed under the Creative Commons Attribution 4.0 International License.

Artikel in diesem Heft

  1. Editorial
  2. Editorial to Volume 10 of ANA
  3. Regular Articles
  4. Convergence Results for Elliptic Variational-Hemivariational Inequalities
  5. Weak and stationary solutions to a Cahn–Hilliard–Brinkman model with singular potentials and source terms
  6. Single peaked traveling wave solutions to a generalized μ-Novikov Equation
  7. Constant sign and nodal solutions for superlinear (p, q)–equations with indefinite potential and a concave boundary term
  8. On isolated singularities of Kirchhoff equations
  9. On the existence of periodic oscillations for pendulum-type equations
  10. Multiplicity of concentrating solutions for a class of magnetic Schrödinger-Poisson type equation
  11. Nehari-type ground state solutions for a Choquard equation with doubly critical exponents
  12. Gradient estimate of a variable power for nonlinear elliptic equations with Orlicz growth
  13. The structure of 𝓐-free measures revisited
  14. Solvability of an infinite system of integral equations on the real half-axis
  15. Positive Solutions for Resonant (p, q)-equations with convection
  16. Concentration behavior of semiclassical solutions for Hamiltonian elliptic system
  17. Global existence and finite time blowup for a nonlocal semilinear pseudo-parabolic equation
  18. On variational nonlinear equations with monotone operators
  19. Existence results for nonlinear degenerate elliptic equations with lower order terms
  20. Blow-up criteria and instability of normalized standing waves for the fractional Schrödinger-Choquard equation
  21. Ground states and multiple solutions for Hamiltonian elliptic system with gradient term
  22. Positivity of solutions to the Cauchy problem for linear and semilinear biharmonic heat equations
  23. Convex solutions of Monge-Ampère equations and systems: Existence, uniqueness and asymptotic behavior
  24. Multiple solutions for critical Choquard-Kirchhoff type equations
  25. Regularity for sub-elliptic systems with VMO-coefficients in the Heisenberg group: the sub-quadratic structure case
  26. Inducing strong convergence of trajectories in dynamical systems associated to monotone inclusions with composite structure
  27. A posteriori analysis of the spectral element discretization of a non linear heat equation
  28. Liouville property of fractional Lane-Emden equation in general unbounded domain
  29. Large data existence theory for three-dimensional unsteady flows of rate-type viscoelastic fluids with stress diffusion
  30. On some classes of generalized Schrödinger equations
  31. Variational formulations of steady rotational equatorial waves
  32. On a class of critical elliptic systems in ℝ4
  33. Exponential stability of the nonlinear Schrödinger equation with locally distributed damping on compact Riemannian manifold
  34. On a degenerate hyperbolic problem for the 3-D steady full Euler equations with axial-symmetry
  35. Existence, multiplicity and nonexistence results for Kirchhoff type equations
  36. Combined effects of Choquard and singular nonlinearities in fractional Kirchhoff problems
  37. Convergence analysis for double phase obstacle problems with multivalued convection term
  38. Multiple solutions for weighted Kirchhoff equations involving critical Hardy-Sobolev exponent
  39. Boundary value problems associated with singular strongly nonlinear equations with functional terms
  40. Global solvability in a three-dimensional Keller-Segel-Stokes system involving arbitrary superlinear logistic degradation
  41. Multiplicity and concentration behaviour of solutions for a fractional Choquard equation with critical growth
  42. Concentration results for a magnetic Schrödinger-Poisson system with critical growth
  43. Periodic solutions for a differential inclusion problem involving the p(t)-Laplacian
  44. The concentration-compactness principles for Ws,p(·,·)(ℝN) and application
  45. Regularity for commutators of the local multilinear fractional maximal operators
  46. An improvement to the John-Nirenberg inequality for functions in critical Sobolev spaces
  47. Local versus nonlocal elliptic equations: short-long range field interactions
  48. Analysis of a diffusive host-pathogen model with standard incidence and distinct dispersal rates
  49. Blowing-up solutions of the time-fractional dispersive equations
  50. Fixed point of some Markov operator of Frobenius-Perron type generated by a random family of point-transformations in ℝd
  51. Non-stationary Navier–Stokes equations in 2D power cusp domain
  52. Non-stationary Navier–Stokes equations in 2D power cusp domain
  53. Nontrivial solutions to the p-harmonic equation with nonlinearity asymptotic to |t|p–2t at infinity
  54. Iterative methods for monotone nonexpansive mappings in uniformly convex spaces
  55. Optimality of Serrin type extension criteria to the Navier-Stokes equations
  56. Fractional Hardy-Sobolev equations with nonhomogeneous terms
  57. New class of sixth-order nonhomogeneous p(x)-Kirchhoff problems with sign-changing weight functions
  58. On the set of positive solutions for resonant Robin (p, q)-equations
  59. Solving Composite Fixed Point Problems with Block Updates
  60. Lions-type theorem of the p-Laplacian and applications
  61. Half-space Gaussian symmetrization: applications to semilinear elliptic problems
  62. Positive radial symmetric solutions for a class of elliptic problems with critical exponent and -1 growth
  63. Global well-posedness of the full compressible Hall-MHD equations
  64. Σ-Shaped Bifurcation Curves
  65. On the critical behavior for inhomogeneous wave inequalities with Hardy potential in an exterior domain
  66. On singular quasilinear elliptic equations with data measures
  67. On the sub–diffusion fractional initial value problem with time variable order
  68. Partial regularity of stable solutions to the fractional Geľfand-Liouville equation
  69. Ground state solutions for a class of fractional Schrodinger-Poisson system with critical growth and vanishing potentials
  70. Initial boundary value problems for the three-dimensional compressible elastic Navier-Stokes-Poisson equations
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